Abstract
The two-dimensional lattice Ginzburg - Landau Hamiltonian is simulated numerically for different values of the coherence length ξ in units of the lattice spacing a, a parameter which controls amplitude fluctuations. The phase diagram on the plane T-ξ is measured. Amplitude fluctuations change dramatically the nature of the phase transition: For values of ξ/a ≃ 1, instead of the smooth Kosterlitz-Thouless transition there is a first-order transition with a discontinuity in the vortex density v and a sharper drop in the helicity modulus Γ. Both observables υ and Γ are analyzed in detail at the crossover region between first and second order which occurs for intermediate values of ξ/a.
Original language | English |
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Pages (from-to) | 399-406 |
Number of pages | 8 |
Journal | Physics Letters, Section A: General, Atomic and Solid State Physics |
Volume | 282 |
Issue number | 6 |
DOIs | |
State | Published - Apr 30 2001 |
Externally published | Yes |
Funding
Work is supported in part by CSIC, Project No. 052, and PEDECIBA.